EP1383116A1 - Procede d'enregistrement optique - Google Patents

Procede d'enregistrement optique Download PDF

Info

Publication number
EP1383116A1
EP1383116A1 EP02713201A EP02713201A EP1383116A1 EP 1383116 A1 EP1383116 A1 EP 1383116A1 EP 02713201 A EP02713201 A EP 02713201A EP 02713201 A EP02713201 A EP 02713201A EP 1383116 A1 EP1383116 A1 EP 1383116A1
Authority
EP
European Patent Office
Prior art keywords
pulse
upward
write
pulses
waveform
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP02713201A
Other languages
German (de)
English (en)
Other versions
EP1383116A4 (fr
Inventor
Tatsuya Kato
Hajime Utsunomiya
Hideki Hirata
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
TDK Corp
Original Assignee
TDK Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by TDK Corp filed Critical TDK Corp
Publication of EP1383116A1 publication Critical patent/EP1383116A1/fr
Publication of EP1383116A4 publication Critical patent/EP1383116A4/fr
Withdrawn legal-status Critical Current

Links

Images

Classifications

    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
    • G11B7/0045—Recording
    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
    • G11B7/006—Overwriting
    • G11B7/0062—Overwriting strategies, e.g. recording pulse sequences with erasing level used for phase-change media
    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
    • G11B20/10—Digital recording or reproducing

Definitions

  • Optical recording media that permits high-density recording and also permits the recorded information to be erased and rewritten have been attracting attention in recent years.
  • the phase-change technology involves irradiating the media with laser beam to change the crystal state of the recording layer to perform recording and detecting the change in the crystalline state of the recording layer accompanying this state change to perform playback.
  • Phase-change type optical recording media is attracting attention because the optical system of the drive is simpler than that for magneto-optical recording media.
  • the recording layer When recording information onto phase-change type optical recording media, the recording layer is irradiated with a high-power (write power) laser until it is above its melting point. Once the recording layer is melted in the portion where the write power is applied, it cools rapidly to form an amorphous write mark.
  • the recording layer when erasing write marks, the recording layer is irradiated with a relatively low-power (erase power) laser which heats it to a temperature above its crystallization temperature but below the melting temperature.
  • erase power When the erase power is applied, recording marks are heated to above their crystallization temperature and then cooled gradually, so they return to the crystalline state. Accordingly, with phase-change type optical recording media, overwriting is possible by modulating the intensity of the same laser beam.
  • the irradiation is performed as a pulse train in order to control the recording mark shape.
  • the specific constitution of this pulse train is called the write waveform.
  • laser diodes take a certain amount of time from when the drive current is applied until their beam intensity reaches the intensity corresponding to that current value, and the laser driver that supplies the drive current to the laser diode takes a certain amount of time to raise the drive current to the stipulated value. Accordingly, even if one attempts to use an extremely short pulse waveform for the laser beam in order to increase the transfer rate, the laser beam intensity corresponding to each pulse attenuates before reaching the recording power. To wit, laser beam emission that strictly conforms to the write waveform cannot be obtained. As a result, the heating of the recording layer is inadequate so the recording marks may be warped in shape or too small, and as a result, jitter in the playback signal may become large or the playback amplitude may become lower.
  • optical recording method that performs recording by irradiating optical recording media with laser beam modulated in intensity based on a write waveform, wherein peak values of upward pulses contained in said write waveform are set based on the respective pulse widths
  • an optical recording method that performs recording by irradiating optical recording media with laser beam modulated in intensity based on a write waveform comprising a top pulse, last pulse and multi-pulses, wherein a peak value of said multi-pulses is set higher than a peak value of said top pulse.
  • a pulse width of said multi-pulses is shorter than a pulse width of said top pulse.
  • a peak value of said top pulse is equal to a peak value of said last pulse.
  • the recording layer 14 consists of phase-change material in which the recording of data is performed by utilizing the difference between its reflectance in the crystalline state and its reflectance in the amorphous state.
  • the laser beam 20 incident from the transparent cover layer 16 is given a pulse waveform having an amplitude from the write power (P w ) to the bottom power (P bo ), thus heating the recording layer 14 to above its melting point, and then the intensity of this laser beam 20 is set to the bottom power (P bo ) for rapid cooling.
  • the region melted by the write power (P w ) is changed to the amorphous state, and this becomes a write mark.
  • the thickness of the recording layer 14 is preferably set to 5-30 nm.
  • the levels of all downward pulses are all set lower than the bias current I bi .
  • the level of the original signal 21a is the write current I w
  • the power of the laser beam 20 generated by the laser diode 23 becomes the write power P w
  • the level of the original signal 21a is the bias current I bi
  • the power of the laser beam 20 generated by the laser diode 23 becomes the write power P bi
  • the level of the original signal 21a is the bottom current I bo
  • the power of the laser beam 20 generated by the laser diode 23 becomes the write power P bo .
  • the drive current waveform of the drive signal 22a generated by the laser driver 22 fundamentally corresponds to the write waveform of the original signal 21a, but a stipulated delay is present in the drive operation of the laser driver 22, so a certain amount of delay occurs with respect to the write waveform. Moreover, there is also a small amount of delay present in the light emission operation of the laser diode 23, so the actual light-emission waveform also has a small amount of delay with respect to the drive current waveform. For this reason, if the upward pulse width of the write waveform is set to be extremely short in order to increase the transfer rate, the laser beam 20 corresponding to the short-width upward pulses attenuates before reaching the recording power. For this reason, laser beam 20 that strictly conforms to the write waveform cannot be obtained. The appearance of this is shown in FIG. 5.
  • fall time is defined to be, when the supply of current to the laser diode 23 by the laser driver 22 is halted (reduced), the time from when the beam intensity becomes 90% of the peak value until the beam intensity becomes 10% of the peak value. Typically, the rise time becomes longer than the fall time. In addition, the aforementioned rise time and fall time are dominated by delay due to the laser driver 22, so the drive current waveform of the laser driver 22 roughly matches the light-emission waveform shown in FIG. 6.
  • the portion corresponding to the multi-pulses within the light-emission waveform also reaches the peak value (P w ), so the recording layer can be adequately heated.
  • these upward pulses are preferably divided into at least two groups depending on the length of their respective T UP .
  • the intensity of the various pulses in the light-emission waveform can be brought to their setpoints (the peak values they should have) or values near thereto.
  • a sample optical recording disc was manufactured by preparing a disc-shaped polycarbonate substrate 120 mm in diameter and 1.2 mm thick with the groove formed simultaneously by injection molding, and forming on its surface a reflective layer, second dielectric layer, recording layer, first dielectric layer and transparent cover layer by the procedure given below.
  • T w was changed depending on the linear velocity in order to make the bit length 0.13 ⁇ m at all linear velocities.

Landscapes

  • Engineering & Computer Science (AREA)
  • Signal Processing (AREA)
  • Optical Recording Or Reproduction (AREA)
  • Optical Head (AREA)
EP02713201A 2001-03-28 2002-03-27 Procede d'enregistrement optique Withdrawn EP1383116A4 (fr)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP2001093743 2001-03-28
JP2001093743A JP4491985B2 (ja) 2001-03-28 2001-03-28 光記録方法
PCT/JP2002/002960 WO2002080153A1 (fr) 2001-03-28 2002-03-27 Procede d'enregistrement optique

Publications (2)

Publication Number Publication Date
EP1383116A1 true EP1383116A1 (fr) 2004-01-21
EP1383116A4 EP1383116A4 (fr) 2008-02-13

Family

ID=18948041

Family Applications (1)

Application Number Title Priority Date Filing Date
EP02713201A Withdrawn EP1383116A4 (fr) 2001-03-28 2002-03-27 Procede d'enregistrement optique

Country Status (7)

Country Link
US (1) US7177254B2 (fr)
EP (1) EP1383116A4 (fr)
JP (1) JP4491985B2 (fr)
KR (1) KR20030083019A (fr)
CN (1) CN1272776C (fr)
TW (1) TW569200B (fr)
WO (1) WO2002080153A1 (fr)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006043211A1 (fr) 2004-10-19 2006-04-27 Koninklijke Philips Electronics N.V. Procede d'ecriture de donnees sur un substrat maitre a des fins d'enregistrement optique

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003123252A (ja) * 2001-10-09 2003-04-25 Hitachi Ltd 情報記録方法および情報記録装置
CN1292410C (zh) * 2002-08-03 2006-12-27 三星电子株式会社 记录/再现信息存储介质的方法
KR100750109B1 (ko) * 2003-02-15 2007-08-21 삼성전자주식회사 정보 저장매체
US20050069002A1 (en) * 2003-09-25 2005-03-31 Hisashi Senga Laser driving device
US7916582B2 (en) * 2004-05-11 2011-03-29 Samsung Electronics Co., Ltd. Optical recording medium, recording/reproducing apparatus and method, initialization method, and reinitialization method
US7663990B2 (en) * 2004-05-21 2010-02-16 Samsung Electronics Co., Ltd. Optical recording medium having access control area and method for recording or reproducing thereof
JP4778287B2 (ja) 2005-09-29 2011-09-21 株式会社日立製作所 情報記録方法及び装置

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0345752A2 (fr) * 1988-06-08 1989-12-13 Hitachi, Ltd. Méthode d'enregistrement d'information optique et appareil et milieu d'enregistrement pour celui-ci
WO2000058775A1 (fr) * 1999-03-29 2000-10-05 T Squared G Incorporated Generateur numerique de formes sinusoidales optiques

Family Cites Families (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2702923B2 (ja) 1987-04-24 1998-01-26 株式会社日立製作所 情報の記録方法及び情報記録装置
JPH01229426A (ja) 1988-03-09 1989-09-13 Matsushita Electric Ind Co Ltd 光学情報の記録方法
JP2669532B2 (ja) * 1988-05-20 1997-10-29 株式会社日立製作所 光ディスク装置
US5590111A (en) * 1990-06-29 1996-12-31 Hitachi, Ltd. Method of controlling recording of optical records
JPH076441A (ja) * 1993-06-17 1995-01-10 Ricoh Co Ltd 光磁気記録方法
JP3171103B2 (ja) 1995-03-31 2001-05-28 三菱化学株式会社 光記録方法および光記録媒体
JP3138610B2 (ja) * 1995-04-13 2001-02-26 株式会社リコー 相変化型光ディスク用記録方法
JPH0964441A (ja) 1995-08-23 1997-03-07 Fujitsu Ltd 発光素子駆動装置
US6751513B1 (en) * 1996-02-16 2004-06-15 Koninklijke Philips Electronics N.V Method and device for recording an optical information carrier
EP0830675B1 (fr) * 1996-02-16 2003-08-06 Koninklijke Philips Electronics N.V. Procede et dispositif d'enregistrement d'un support d'informations optique
KR100505796B1 (ko) * 1997-02-14 2005-10-19 코닌클리케 필립스 일렉트로닉스 엔.브이. 광기록매체의기록방법및기록장치
JP3456121B2 (ja) * 1997-09-09 2003-10-14 三菱電機株式会社 レーザダイオード用電源制御装置
JP3323782B2 (ja) * 1997-09-09 2002-09-09 株式会社日立製作所 情報の記録方法
JP2000215449A (ja) * 1999-01-27 2000-08-04 Taiyo Yuden Co Ltd 光情報記録方法及びその装置
JP4268312B2 (ja) * 1999-04-28 2009-05-27 パナソニック株式会社 光学的記録再生装置
JP2000322740A (ja) * 1999-05-12 2000-11-24 Ricoh Co Ltd 光記録媒体及びその記録方法
JP2001134943A (ja) * 1999-11-05 2001-05-18 Yamaha Corp 光ディスク記録装置のプッシュプル信号処理回路およびウォブル抽出回路ならびにプリピット検出回路
EP1117094B1 (fr) * 2000-01-17 2012-11-21 Mitsubishi Kagaku Media Co., Ltd. Méthode d'enregistrement pour un support d'enregistrement à changement de phase
JP3730084B2 (ja) * 2000-05-19 2005-12-21 パイオニア株式会社 光制御回路

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0345752A2 (fr) * 1988-06-08 1989-12-13 Hitachi, Ltd. Méthode d'enregistrement d'information optique et appareil et milieu d'enregistrement pour celui-ci
WO2000058775A1 (fr) * 1999-03-29 2000-10-05 T Squared G Incorporated Generateur numerique de formes sinusoidales optiques

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See also references of WO02080153A1 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006043211A1 (fr) 2004-10-19 2006-04-27 Koninklijke Philips Electronics N.V. Procede d'ecriture de donnees sur un substrat maitre a des fins d'enregistrement optique

Also Published As

Publication number Publication date
WO2002080153A1 (fr) 2002-10-10
EP1383116A4 (fr) 2008-02-13
KR20030083019A (ko) 2003-10-23
CN1272776C (zh) 2006-08-30
US7177254B2 (en) 2007-02-13
JP2002298349A (ja) 2002-10-11
JP4491985B2 (ja) 2010-06-30
TW569200B (en) 2004-01-01
US20030063540A1 (en) 2003-04-03
CN1535464A (zh) 2004-10-06

Similar Documents

Publication Publication Date Title
US6842415B2 (en) Information recording method and apparatus with suppressed mark edge jitters
US7068591B2 (en) Information recording method and optical recording medium therefor
US7384678B2 (en) Optical recording medium and process for producing the same, sputtering target, using process of optical recording medium, and optical recording apparatus
JP2002245624A (ja) 光記録方法、光記録装置および光記録媒体
TW200421334A (en) Phase change type optical recording medium and recording method therefor
US7177254B2 (en) Optical recording method for high transfer rates
CN100449617C (zh) 用于相变型光记录介质的记录方法
EP1638092B1 (fr) Procédé d'enregistrement d'informations sur un support d'enregistrement optique, et appareil d'enregistrement et de reproduction d'informations
JP2001344763A (ja) 光記録方法、光記録装置および光記録媒体
US6438085B1 (en) Optical recording method
US20060262697A1 (en) Medium and method for providing a desirable direct overwriting characteristic for optical data recorded at different linear recording velocities
WO2002043058A1 (fr) Procede d'inspection et procede de production d un moyen d'enregistrement optique
EP1612779B1 (fr) Procédé d'enregistrement sur des supports d'enregistrement optiques, et dispositif d'enregistrement optique
US6560182B1 (en) Optical recording method
US6456576B1 (en) Optical recording method
US20050041568A1 (en) Optical recording medium and method of recording information to optical recording medium
KR100327223B1 (ko) 고밀도기록에적합한기록방법
JP2003030836A (ja) 情報の記録方法、情報記録媒体及び情報記録装置
JP2004030820A (ja) レーザビーム強度決定方法、これに用いる臨界値の生成方法、オーバーライト回数決定プログラム及び光記録媒体
US7680010B2 (en) Method for recording information on optical recording medium
JP2003136840A (ja) 光情報記録媒体
KR19990057705A (ko) 상변화형 광디스크
KR19990057704A (ko) 상변화형 광디스크

Legal Events

Date Code Title Description
PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

17P Request for examination filed

Effective date: 20030930

AK Designated contracting states

Kind code of ref document: A1

Designated state(s): AT BE CH CY DE DK ES FI FR GB GR IE IT LI LU MC NL PT SE TR

A4 Supplementary search report drawn up and despatched

Effective date: 20080111

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION HAS BEEN WITHDRAWN

18W Application withdrawn

Effective date: 20080317